about
Enhanced superconductivity accompanying a Lifshitz transition in electron-doped FeSe monolayer.Experimental evidence of hourglass fermion in the candidate nonsymmorphic topological insulator KHgSb.Local antiferromagnetic exchange and collaborative Fermi surface as key ingredients of high temperature superconductors.Electronic structure of SrSn2As2 near the topological critical pointMagnetic moment evolution and spin freezing in doped BaFe2As2Fermi surface and effective masses in photoemission response of the (Ba1-x K x )Fe2As2 superconductor.Observation of topological superconductivity on the surface of an iron-based superconductor.Spectroscopic evidence for a pseudogap in the normal state of underdoped high-T c superconductorsMicroscopic electronic inhomogeneity in the high-Tc superconductor Bi2Sr2CaCu2O8+xThe origin of multiple superconducting gaps in MgB2Effect of Li-deficiency impurities on the electron-overdoped LiFeAs superconductorEvidence for Majorana bound states in an iron-based superconductorA distinct bosonic mode in an electron-doped high-transition-temperature superconductorFermi surface dichotomy of the superconducting gap and pseudogap in underdoped pnictidesEvolution from incoherent to coherent electronic states and its implications for superconductivity inFeTe1−xSexAngle-resolved photoemission observation of isotropic superconducting gaps in isovalent Ru-substituted Ba(Fe0.75Ru0.25)2As2Experimental Investigation of the Electronic Structure of Ca0.83La0.17Fe2As2Effects of Ru substitution on electron correlations and Fermi-surface dimensionality in Ba(Fe1−xRux)2As2Isotropic superconducting gaps with enhanced pairing on electron Fermi surfaces in FeTe0.55Se0.45Orbital characters determined from Fermi surface intensity patterns using angle-resolved photoemission spectroscopyQuasinested Fe orbitals versus Mott-insulating V orbitals in superconductingSr2VFeAsO3as seen from angle-resolved photoemissionUnconventional superconducting gap inNaFe0.95Co0.05Asobserved by angle-resolved photoemission spectroscopyObservation of an isotropic superconducting gap at the Brillouin zone centre of Tl0.63K0.37Fe1.78Se2Dirac nodal surfaces and nodal lines in ZrSiSMomentum distribution sum rule for angle-resolved photoemissionGap anisotropy in Bi2Sr2CaCu2O8+ delta by ultrahigh-resolution angle-resolved photoemissionElectronic structure of organic superconductors kappa -(ET)2CuSuperconducting energy gap in Bi1.8Pb0.4Sr2Ca2Cu3O10+ delta studied by photoemission spectroscopyUnusual electronic structure near EF in the organic superconductor kappa -Phenomenological models for the gap anisotropy of Bi2Sr2CaCu2O8 as measured by angle-resolved photoemission spectroscopyPolarization selection rules and superconducting gap anisotropy in Bi2Sr2CaCu2O8Quasiparticle line shape of Sr2RuO4 and its relation to anisotropic transportCorrelating off-stoichiometric doping and nanoscale electronic inhomogeneity in the high-Tc superconductor Bi2Sr2CaCu2O8+deltaARPES on Na0.6CoO2: Fermi surface and unusual band dispersionFermi surface topology of Ca1.5Sr0.5RuO4 determined by angle-resolved photoelectron spectroscopyElectron correlation and fermi surface topology of NaxCoO2Angle-resolved photoemission spectroscopy of the antiferromagnetic superconductor Nd1.87Ce0.13CuO4: anisotropic spin-correlation gap, pseudogap, and the induced quasiparticle mass enhancementCompetition between antiferromagnetism and superconductivity in the electron-doped cuprates triggered by oxygen reductionTwo- to three-dimensional crossover in the electronic structure of (Bi, Pb)2(Sr, La)2CuO(6+delta) from angle-resolved photoemission spectroscopyCoexistence of competing orders with two energy gaps in real and momentum space in the high temperature superconductor Bi_{2}Sr_{2-x}La_{x}CuO_{6+delta}
P50
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P50
description
angle-resolved photoelectron spectroscopist at the CAS Institute of Physics
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wetenschapper
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name
H. Ding
@ast
H. Ding
@es
H. Ding
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Hong Ding
@en
type
label
H. Ding
@ast
H. Ding
@es
H. Ding
@nl
Hong Ding
@en
prefLabel
H. Ding
@ast
H. Ding
@es
H. Ding
@nl
Hong Ding
@en
P108
P106
P1153
8337837900
P21
P31
P496
0000-0003-4422-9248